Evolution of plastic anisotropy for high-strain-rate computations

A model for anisotropic material strength, and for changes in the anisotropy due to plastic strain, is described. This model has been developed for use in high-rate, explicit, Lagrangian multidimensional continuum-mechanics codes. The model handles anisotropies, in single-phase materials, in particu...

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Veröffentlicht in:Computer methods in applied mechanics and engineering 1997-04, Vol.143 (3), p.249-270
Hauptverfasser: Schiferl, Sheila K., Maudlin, Paul J.
Format: Artikel
Sprache:eng
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Zusammenfassung:A model for anisotropic material strength, and for changes in the anisotropy due to plastic strain, is described. This model has been developed for use in high-rate, explicit, Lagrangian multidimensional continuum-mechanics codes. The model handles anisotropies, in single-phase materials, in particular the anisotropies due to crystallographic texture—preferred orientations of the single-crystal grains. Textural anisotropies, and the changes in these anisotropies, depend overwhelmingly on the crystal structure of the material and on the deformation history. The changes, particularly for complex deformations, are not amenable to simple analytical forms. To handle this problem, the material model described here includes a texture code, or micromechanical calculation, coupled to a continuum code. The texture code updates grain orientations as a function of tensor plastic strain, and calculates the yield strength in different directions. A yield function is fitted to these yield ‘points’. For each computational cell in the continuum simulation, the texture code tracks a particular set of grain orientations. The orientations will change due to the tensor strain history, and the yield function will change accordingly. Hence, the continuum code supplies a tensor strain to the texture code, and the texture code supplies an updated yield function to the continuum code. Since significant texture changes require relatively large strains—typically, a few percent or more—the texture code is not called very often, and the increase in computer time is not excessive. The model was implemented, using a finite-element continuum code and a texture code specialized for hexagonal-close-packed crystal structures. The results for several uniaxial stress problems and an explosive-forming problem are shown.
ISSN:0045-7825
1879-2138
DOI:10.1016/S0045-7825(96)01159-0